A Further Study on Large Size LSO and LYSO Crystal Samples
|
|
- Sabrina Hall
- 5 years ago
- Views:
Transcription
1 October 25, 2005 IEEE NSS, N12-6, Puerto-Rico 1 A Further Study on Large Size LSO and LYSO Crystal Samples Jianming Chen, Liyuan Zhang, Ren-yuan Zhu California Institute of Technology
2 BGO, LSO & LYSO Samples % Ce in LSO/LYSO, 5--10% yttrium fraction in LYSO Cube: 1.7 cm (1.5 X 0 ), Bar: 2.5 x 2.5 x 20 cm (18 X 0 ) SIC BGO CPI LYSO Saint-Gobain LYSO CTI LSO 2
3 Experiment Without any thermal treatment, all samples went through measurement for optical and scintillation properties. Optical properties measured: transmittance, emission and excitation spectra. Light output and light response uniformity were measured with PMT and Si APD readout. Radiation induced phosphorescence intensity was measured for two LYSO long samples under γ ray irradiation, which was used to estimate readout noise with 100 ns gate. 3
4 Excitation, Emission & Transmittance Identical transmittance, emission & excitation spectra Part of emitted light is self-absorbed in long samples 1.7 cm Cube 2.5 x 2.5 x 20 cm Bar 4
5 CTI LSO: longitudinal optical uniformity No longitudinal variation in optical properties Transverse transmittance approaches theoretical limit 5
6 Emission Weighted Q.E. Areas under emission spectra proportional to the LY 59%/75% QE for LSO/LYSO readout with Si PD/APD 6
7 PMT Based Readout with Coincidence Systematic error with repeated mounts & measurements: < 1% 7
8 137 Cs & 22 Na Pulse Height Spectra Cube and bar samples have 8% and 10% FWHM resolution respectively for 137 Cs (0.66 MeV) and 22 Na source (0.51 MeV) CPI LYSO bar has double peak because of poor annealing Cube Bar 8
9 Light Output & Decay Time LSO/LYSO Light yield: a factor of 4/100 of BGO/PWO LSO/LYSO decay time: 42 ns compared to 300 ns of BGO Cube Bar 9
10 APD Based Readout with Coincidence Two Hamamatsu S APD, Canberra 2003 BT preamplifier and ORTEC 673 shaping amplifier with shaping time 250 ns Hamamatsu S APD 10
11 APD Readout Calibration Readout noise: 67 electrons for 2 APD with 250 ns shaping Systematic error with repeated mountings & measurements: 2.4% Calibration with Fe-55 source: 2.38 electrons/adc Channel 11
12 Pulse Height & Light Yield with APDs Na-22 annihilation peak (510 kev) well measured CTI LSO sample has significantly higher LO 12
13 LSO Light Response Uniformity Uniformity depends on end coupled to the PMT/APD, indicating a not uniform light yield along crystal 13
14 LYSO LRU Measured with APD Uniformity depends on which end coupled to the APD, indicating a not uniform light yield along crystal 14
15 γ ray Induced Readout Noise Sample L.Y. F Q 15 rad/h Q 500 rad/h σ 15 rad/h σ 500 rad/h ID p.e./mev μa/rad/h p.e. p.e. MeV MeV CPI 1, x x SG 1, x x γ ray induced PMT anode current can be converted to the photoelectron numbers (Q) integrated in 100 ns gate. Its statistical fluctuation contributes to the readout noise (σ). 15
16 CMS PWO Resolution 77k PWO Designed Resolution Energy Resolution: σ(e)/e < 1% if E > 25 GeV σ(e)/e ~ 0.5% at 120 GeV 2004 SM Beam Test Monitoring: 0.04% 16
17 LSO/LYSO ECAL Performance Less demanding to the environment because of small temperature coefficient. Radiation damage is less an issue as compared to the CMS PWO ECAL. A better energy resolution, σ(e)/e, at low energies than L3 BGO and CMS PWO because of its high light output and low readout noise: % / E 0.55% /E / E 17
18 Summary Ce doped LSO & LYSO crystals have fast (42 ns) and high (4 X BGO) light output. The light output of 2.5 x 2.5 x 20 cm LSO and LYSO samples, excited by 0.51 MeV γ ray, can be readout by Hamamatsu S APD (2 x 0.25 cm 2 ) with electronic noise of 70 electrons (< 35 kev). Longitudinal light response uniformity of long LSO/LYSO samples seems affected by Ce distribution along crystal. The radiation induced phosphorescence in 2.5 x 2.5 x 20 cm LYSO causes ~0.2 MeV 15 rad/h. An LSO/LYSO crystal calorimeter would provide very good energy resolution down to MeV range for future HEP experiments. To be understood: why LSO long sample has higher LO as compared to long LYSO samples with APD readout. 18
19 Possible Origin of Non Uniformity C. Melcher: LO in LSO is a function of Ce concentration B. Chai: LO in LYSO is a function of atomic fraction of Yttrium 19
Cherenkov Radiation. Doctoral Thesis. Rok Dolenec. Supervisor: Prof. Dr. Samo Korpar
Doctoral Thesis Time-of-Flight Time-of-Flight Positron Positron Emission Emission Tomography Tomography Using Using Cherenkov Cherenkov Radiation Radiation Rok Dolenec Supervisor: Prof. Dr. Samo Korpar
More informationThe Progress of TOF on BESIII
The Progress of TOF on BESIII Yuekun Heng 1, Chong Wu 1, Zhijia Sun 1, Li Zhao 1,2, Cheng Li 2, Qi An 2, Shubin Liu 2, Jinjie Wu 2, Yuda Zhao 1,3, Fengmei Wang 1,4, Xiaojian Zhao 1, Feng Shi 1, Zhenghua
More informationSiPMs for Čerenkov imaging
SiPMs for Čerenkov imaging Peter Križan University of Ljubljana and J. Stefan Institute Trends in Photon Detectors in Particle Physics and Calorimetry, Trieste, June 2-4, 2008 Contents Photon detectors
More informationAX-PET : A novel PET concept with G-APD readout
AX-PET : A novel PET concept with G-APD readout Matthieu Heller CERN - PH/DT Marie Curie network MC-PAD Matthieu.heller@cern.ch On behalf of the AX-PET collaboration https://twiki.cern.ch/twiki/bin/view/axialpet
More informationHHS Public Access Author manuscript Phys Med Biol. Author manuscript; available in PMC 2016 February 19.
Monte Carlo calculations of PET coincidence timing: single and double-ended readout Stephen E Derenzo, Woon-Seng Choong, and William W Moses Life Sciences Division, Lawrence Berkeley National Laboratory,
More informationThe LHCb upgrade. Outline: Present LHCb detector and trigger LHCb upgrade main drivers Overview of the sub-detector modifications Conclusions
The LHCb upgrade Burkhard Schmidt for the LHCb Collaboration Outline: Present LHCb detector and trigger LHCb upgrade main drivers Overview of the sub-detector modifications Conclusions OT IT coverage 1.9
More informationScintillators and photodetectors. 1. Generation of Optical Photons 2. Transport of Optical Photons 3. Detection of Optical Photons
Scintillators and photodetectors 1. Generation of Optical Photons 2. Transport of Optical Photons 3. Detection of Optical Photons 1) Generation of Optical Photons A) Organic (molecular) scintillators Advantages:
More informationDevelopment of LYSO Detector Modules for an EDM Polarimeter at COSY. for the JEDI Collaboration
Mitglied der Helmholtz-Gemeinschaft Development of LYSO Detector Modules for an EDM Polarimeter at COSY for the JEDI Collaboration February 28, 2018 DPG Spring Meeting, PhD @ SMART EDM_Lab, TSU, Georgia
More informationTORCH: A large-area detector for precision time-of-flight measurements at LHCb
TORCH: A large-area detector for precision time-of-flight measurements at LHCb Neville Harnew University of Oxford ON BEHALF OF THE LHCb RICH/TORCH COLLABORATION Outline The LHCb upgrade TORCH concept
More informationUsing only HyCal. Graph. Graph
Live charge weighted ep yield from all the 2GeV empty target runs Scattering angle from.7 to.9 deg, background dominated by upstream collimator (8%) Notice that here uncertainty from the live charge measurement
More informationFuture Prospects of Time-of-Flight PET: Scintillator, Detector and Depth-of- interaction (DOI) Technologies. TOF scanners. Clinical benefit of TOF PET
Future Prospects of Time-of-Flight PET: Scintillator, Detector and Depth-of- interaction (DOI) Technologies Suleman Surti Physics & Instrumentation Group Department of Radiology University of Pennsylvania
More informationIn-vivo dose verification for particle therapy
In-vivo dose verification for particle therapy D.R. Schaart, NCS Lustrum, 5-Oct-2012 HollandPTC 1 Protons vs. photons Photons Protons Dennis R. Schaart Delft University of Technology 2 Protons: the promise
More informationin PET Medical Imaging
Fast Timing and TOF in PET Medical Imaging William W. Moses Lawrence Berkeley National Laboratory October 15, 2008 Outline: Time-of-Flight PET History Present Status Future This work was supported in part
More informationFast Timing and TOF in PET Medical Imaging
Fast Timing and TOF in PET Medical Imaging William W. Moses Lawrence Berkeley National Laboratory October 15, 2008 Outline: Time-of-Flight PET History Present Status Future This work was supported in part
More informationMedical Imaging BMEN Spring 2016
Name Medical Imaging BMEN 420-501 Spring 2016 Homework #4 and Nuclear Medicine Notes All questions are from the introductory Powerpoint (based on Chapter 7) and text Medical Imaging Signals and Systems,
More informationarxiv:physics/ v1 [physics.ins-det] 18 Dec 1998
Studies of 1 µm-thick silicon strip detector with analog VLSI readout arxiv:physics/981234v1 [physics.ins-det] 18 Dec 1998 T. Hotta a,1, M. Fujiwara a, T. Kinashi b, Y. Kuno c, M. Kuss a,2, T. Matsumura
More informationExtremely Fast Detector for 511 kev Gamma
Extremely Fast Detector for 511 kev Gamma V. Sharyy, D. Yvon, G. Tauzin, E.Delagnes, Ph. Abbon, J P. Bard, M. Kebbiri, M. Alokhina, C. Canot IRFU, CEA D. Breton, J. Maalmi LAL,IN2P3 Journée 2015 du Labex
More informationCorso di laurea in Fisica A.A Fisica Medica 5 SPECT, PET
Corso di laurea in Fisica A.A. 2007-2008 Fisica Medica 5 SPECT, PET Step 1: Inject Patient with Radioactive Drug Drug is labeled with positron (β + ) emitting radionuclide. Drug localizes
More information218 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 44, NO. 2, APRIL 1997
218 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 44, NO. 2, APRIL 1997 Compton Scatter and X-ray Crosstalk and the Use of Very Thin Intercrystal Septa in High-Resolution PET Detectors Craig S. Levin, Member,
More informationFront end electronics and system design for the NUSTAR experiments at the FAIR facility. FEE 2006 Workshop
Front end electronics and system design for the NUSTAR experiments at the FAIR facility Presented by Ian Lazarus on behalf of NUSTAR collaboration FEE 2006 Workshop Ian Lazarus NPG, CCLRC Daresbury Overview
More information8/3/2016. Outline. The EPID Strikes Back: Future EPID Technology and Applications. Active Matrix Flat-Panel Imagers (AMFPIs)
8//6 The EPID Strikes Back: Future EPID Technology and Applications Larry E. Antonuk Department of Radiation Oncology University of Michigan, Ann Arbor Acknowledgements: Youcef El-Mohri, Qihua Zhao (U.
More informationLarge Plastic Scintillation Detectors for the Nuclear Materials Identification System
Large Plastic Scintillation Detectors for the Nuclear Materials Identification System J.S. Neal, J.T. Mihalczo, M. T. Hiatt, J. D. Edwards Oak Ridge National Laboratory P. O. Box 2008, Oak Ridge, Tennessee
More informationIntroduction to Positron Emission Tomography
Planar and SPECT Cameras Summary Introduction to Positron Emission Tomography, Ph.D. Nuclear Medicine Basic Science Lectures srbowen@uw.edu System components: Collimator Detector Electronics Collimator
More informationDigital Filters in Radiation Detection and Spectroscopy
Digital Filters in Radiation Detection and Spectroscopy Digital Radiation Measurement and Spectroscopy NE/RHP 537 1 Classical and Digital Spectrometers Classical Spectrometer Detector Preamplifier Analog
More informationCharacterization of a Time-of-Flight PET Scanner based on Lanthanum Bromide
2005 IEEE Nuclear Science Symposium Conference Record M04-8 Characterization of a Time-of-Flight PET Scanner based on Lanthanum Bromide J. S. Karp, Senior Member, IEEE, A. Kuhn, Member, IEEE, A. E. Perkins,
More informationCHAPTER 11 NUCLEAR MEDICINE IMAGING DEVICES
CHAPTER 11 M.A. LODGE, E.C. FREY Russell H. Morgan Department of Radiology and Radiological Sciences, Johns Hopkins University, Baltimore, Maryland, United States of America 11.1. INTRODUCTION Imaging
More informationDeliverable D10.2. WP10 JRA04 INDESYS Innovative solutions for nuclear physics detectors
MS116 Characterization of light production, propagation and collection for both organic and inorganic scintillators D10.2 R&D on new and existing scintillation materials: Report on the light production,
More informationAn educational tool for demonstrating the TOF-PET technique
Nuclear Instruments and Methods in Physics Research A 471 (2001) 200 204 An educational tool for demonstrating the TOF-PET technique T.Bȧack a, *, J. Cederkȧall a, B. Cederwall a, A. Johnson a, A. Kerek
More informationA New Model for Optical Crosstalk in SinglePhoton Avalanche Diodes Arrays
A New Model for Optical Crosstalk in SinglePhoton Avalanche Diodes Arrays I. Rech, A. Ingargiola, R. Spinelli, S. Marangoni, I. Labanca, M. Ghioni, S. Cova Dipartimento di Elettronica ed Informazione Politecnico
More informationX-Ray fluorescence and Raman spectroscopy
X-Ray fluorescence and Raman spectroscopy Advanced physics laboratory (nd part) 4CFU Catalini Letizia, De Angelis Giulia Vittoria, Piselli Verdiana Abstract In this paper we report about two different
More informationDevelopment of Ultrafast CXRS system in Heliotron J. Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016
1 Development of Ultrafast CXRS system in Heliotron J Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016 2 Outline 1. Introduction 2. Charge exchange Recombination Spectroscopy (CXRS)
More informationWork in Tbilisi. David Mchedlishvili (SMART EDM_lab of TSU) GGSWBS , Tbilisi. Shota Rustaveli National Science Foundation
Mitglied der Helmholtz-Gemeinschaft David Mchedlishvili (SMART EDM_lab of TSU) Work in Tbilisi GGSWBS 18 23.08.2018, Tbilisi JEDI: Charged-Particle EDM Search Main principle: Inject polarized particles
More informationTiming properties of MCP-PMT
Photon Detector Workshop at Kobe, 27-29 June 27 Timing properties of MCP-PMT - Time resolution - Lifetime - Rate dependence K.Inami (Nagoya university, Japan) Introduction Photon device for TOP counter
More informationGoals of this presentation
Transferring HEP Innovative concepts of electronics, trigger and DAQ Architecture for future large experiments to state of the art applications in medical imaging. P. Le Dû p.ledu@ipnl.in2p3.fr DEC_2010
More informationInterpolating Silicon Photomultipliers
Interpolating Silicon Photomultipliers Peter Fischer, Heidelberg University, Germany (Presenter) Claudio Piemonte, FBK, Italy We present the novel Interpolating Silicon PhotoMultiplier (ISiPM) topology
More informationMeasuring Reflective Properties of PTFE for Applications in Liquid Xenon Detectors
Measuring Reflective Properties of PTFE for Applications in Liquid Xenon Detectors Catherine Lussenhop Columbia University, Department of Physics August 6, 2010 Abstract The XENON100 experiment uses 161kg
More informationDelayline Detectors. Imaging Detection of Electrons, Ions & Photons with Picosecond Time Resolution. e - I +
Delayline Detectors Imaging Detection of Electrons, Ions & Photons with Picosecond Time Resolution e - I + Delayline Readout of MCPs - The Technical Approach - Microchannel-Plate (MCP) detectors provide
More informationThis section gives a brief description of the MatrixB system outlining its main features and applications.
Modular Scintillator Readout Solution for Nuclear Medicine Document Overview This document provides the user with a comprehensive description of the hardware and software provided in the SensL Matrix readout
More informationPositron Emission Tomography
Physics 656 Seminar on Physical Fundamentals of Medical Imaging Positron Emission Tomography Ahmed Qamesh Outline What is PET? PET mechanism Radionuclide and its synthesis Detection concept and Development
More informationApplication of MCNP Code in Shielding Design for Radioactive Sources
Application of MCNP Code in Shielding Design for Radioactive Sources Ibrahim A. Alrammah Abstract This paper presents three tasks: Task 1 explores: the detected number of as a function of polythene moderator
More informationThe AMS-02 Anticoincidence Counter. Philip von Doetinchem I. Phys. Inst. B, RWTH Aachen for the AMS-02 Collaboration DPG, Freiburg March 2008
I. Phys. Inst. B, RWTH Aachen for the AMS-02 Collaboration DPG, Freiburg March 2008 Cosmic Rays in the GeV Range world average SUSY DM KK DM good agreement of data and propagation models, but some unexplained
More informationWe are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists. International authors and editors
We are IntechOpen, the world s leading publisher of Open Access books Built by scientists, for scientists 3,500 108,000 1.7 M Open access books available International authors and editors Downloads Our
More informationSection 2 PROGRESS IN LASER FUSION
Section 2 PROGRESS IN LASER FUSION 2.A Optical Fiducials for X-Ray Streak Cameras X-ray streak cameras are the primary instruments for studying the transient nature of laser-produced plasmas. However,
More informationSupporting information for: A highly directional room-temperature single. photon device
Supporting information for: A highly directional room-temperature single photon device Nitzan Livneh,, Moshe G. Harats,, Daniel Istrati, Hagai S. Eisenberg, and Ronen Rapaport,, Applied Physics Department,
More informationEffects of system geometry and other physical factors on photon sensitivity of high-resolution
Home Search Collections Journals About Contact us My IOPscience Effects of system geometry and other physical factors on photon sensitivity of high-resolution positron emission tomography This article
More informationIntroduction to Biomedical Imaging
Alejandro Frangi, PhD Computational Imaging Lab Department of Information & Communication Technology Pompeu Fabra University www.cilab.upf.edu X-ray Projection Imaging Computed Tomography Digital X-ray
More informationProject GAMMA: Adaptive Methods for Medical Applications
Project GAMMA: Adaptive Methods for Medical Applications V. Solovov, A. Morozov, V. Chepel, V. Domingos, R.Martins, L. Pereira, F. Neves, A. Lindote, F. Fraga, I.Lopes, F. Alves LIP-Coimbra and Coimbra
More informationPSA Performance Analysis and Optimization
AGATA Week Madrid 2014 IKP Cologne 23. Januar 2014 Content Introduction 1 Introduction 2 3 Introduction PSA performance within specifications but: Systematic errors Non isotropic distribution of hits with
More informationFPGA based charge fast histogramming for GEM detector
FPGA based charge fast histogramming for GEM detector Krzysztof T. Pozniak a, A. Byszuk a, M. Chernyshova b, R. Cieszewski a, T. Czarski b, W. Dominik c, K. Jakubowska b, G. Kasprowicz a, J. Rzadkiewicz
More informationSCINTILLATORS-SiPM COUPLING
SCINTILLATORS-SiPM COUPLING G.FELICI LNF-INFN SCINTILLATOR ßàSIPM 1 st PROBLEM: EJ-200 peak emission spectrum do not match S18825 peak sensitivity AMPLITUDE 1.0 0.8 0.6 0.4 0.2 EJ-200 EMISSION SPECTRUM
More informationDiagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology
Diagnostic imaging techniques Krasznai Zoltán University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology 1. Computer tomography (CT) 2. Gamma camera 3. Single Photon
More informationNuclear Instruments and Methods in Physics Research A
Nuclear Instruments and Methods in Physics Research A 621 (2010) 590 594 Contents lists available at ScienceDirect Nuclear Instruments and Methods in Physics Research A journal homepage: www.elsevier.com/locate/nima
More information8/2/2017. Disclosure. Philips Healthcare (Cleveland, OH) provided the precommercial
8//0 AAPM0 Scientific Symposium: Emerging and New Generation PET: Instrumentation, Technology, Characteristics and Clinical Practice Aug Wednesday 0:4am :pm Solid State Digital Photon Counting PET/CT Instrumentation
More informationThe Monte Carlo simulation of a Package formed by the combination of three scintillators: Brillance380, Brillance350, and Prelude420.
EURONS I3 506065 JRA9 RHIB Report made during stay IEM-CSIC Madrid december 2006 MINISTERIO DE ASUNTOS EXTERIORES Y DE COOPERACIÓN AECI VICESECRETARÍA GENERAL The Monte Carlo simulation of a Package formed
More informationDevelopment of automated ultraviolet laser beam profiling system using fluorometric technique
Development of automated ultraviolet laser beam profiling system using fluorometric technique BB Shrivastava*, NS Benerji, P Bhatnagar, HS Vora a and U Nundy Chemical and Excimer Laser Section a Laser
More informationEUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH CERN PH EP/2004 050 19 August 2004 Novel Geometrical Concept of a High Performance Brain PET Scanner - Principle, Design and Performance Estimates J. Séguinot
More informationhsfc pro 12bit ultra speed intensified imaging
hsfc pro 12bit ultra speed intensified imaging four MCP-image intensifier camera modules ultra fast shutter down to 3ns (optional 1.5ns) in single mode excellent sensitivity of the system allows single
More informationContinuation Format Page
C.1 PET with submillimeter spatial resolution Figure 2 shows two views of the high resolution PET experimental setup used to acquire preliminary data [92]. The mechanics of the proposed system are similar
More informationPMT Candidates for SSD Challenge for PMTs in air-shower detection highest linear dynamic range
PMT Candidates for SSD Challenge for PMTs in air-shower detection highest linear dynamic range Karl-Heinz Becker, Karl-Heinz Kampert, Alex Kääpä, Christian Pauly, Sven Querchfeld, Julian Rautenberg OBSERVATORY
More informationObtainment of Prototypical images and Detector performance simulations. Guillaume Potdevin for the XFEL-HPAD-Consortium
Obtainment of Prototypical images and Detector performance simulations Overview of the analysis Outlook Prototypical images: Single object imaging & XPCS short presentation (reminder ) Presentation of
More informationUCS-20. Operating Manual Macintosh Edition. Spectrum Techniques, Inc. Oak Ridge, Tennessee USA. Universal Computer Spectrometer.
UCS-20 Universal Computer Spectrometer Operating Manual Macintosh Edition April 2004 Spectrum Techniques, Inc. Oak Ridge, Tennessee USA. TABLE OF CONTENTS Overview Software Disk Menus File Edit Mode Calculations
More informationProgress in FDIRC & TOF
Progress in FDIRC & TOF J. Va vra, SLAC Content FDIRC prototype - Activities related to analysis of the last test beam run TOF detector - Summary of test results Next steps Appendix - PID electronics summary
More informationUCS 10. Operating Manual. Spectrum Techniques, Inc. Oak Ridge, Tenn. USA. Universal Computer Spectrometer. August 1996
UCS 10 Universal Computer Spectrometer Operating Manual August 1996 Spectrum Techniques, Inc. Oak Ridge, Tenn. USA. TABLE OF CONTENTS Overview Software Disk Menus File Edit Mode Calculations Tools Settings
More informationIntroduction to Emission Tomography
Introduction to Emission Tomography Gamma Camera Planar Imaging Robert Miyaoka, PhD University of Washington Department of Radiology rmiyaoka@u.washington.edu Gamma Camera: - collimator - detector (crystal
More informationLimitations in the PHOTON Monte Carlo gamma transport code
Nuclear Instruments and Methods in Physics Research A 480 (2002) 729 733 Limitations in the PHOTON Monte Carlo gamma transport code I. Orion a, L. Wielopolski b, * a St. Luke s/roosevelt Hospital, Columbia
More informationModeling the ORTEC EX-100 Detector using MCNP
Modeling the ORTEC EX-100 Detector using MCNP MCNP is a general-purpose Monte Carlo radiation transport code for modeling the interaction of radiation with materials based on composition and density. MCNP
More informationUpdate on Energy Resolution of
Update on Energy Resolution of the EMC Using µµγ Sample David Hopkins Royal Holloway, University of London EMC Reconstruction Workshop, December 5 th, 2004 Outline Study of photon energy resolution Compare
More informationUniformity scan of the 6cm tubes. Jingbo Wang Argonne National Laboratory, Lemont, IL
Uniformity scan of the 6cm tubes Jingbo Wang Argonne National Laboratory, Lemont, IL wjingbo@anl.gov Update of the test system Realized the computer control for the multi-channel HV supply, the 2D translation
More informationNEAR-IR BROADBAND POLARIZER DESIGN BASED ON PHOTONIC CRYSTALS
U.P.B. Sci. Bull., Series A, Vol. 77, Iss. 3, 2015 ISSN 1223-7027 NEAR-IR BROADBAND POLARIZER DESIGN BASED ON PHOTONIC CRYSTALS Bogdan Stefaniţă CALIN 1, Liliana PREDA 2 We have successfully designed a
More informationTime-of-Flight Technology
Medical Review Time-of-Flight Technology Bing Bai, PhD Clinical Sciences Manager, PET/CT Canon Medical Systems INTRODUCTION Improving the care for every patient while providing a high standard care to
More informationAnalogue, Digital and Semi-Digital Energy Reconstruction in the CALICE AHCAL
Analogue, Digital and Semi-Digital Energy Reconstruction in the AHCAL Deutsches Elektronen Synchrotron (DESY), Hamburg, Germany E-mail: coralie.neubueser@desy.de Within the collaboration different calorimeter
More information5 th HERD workshop CERN. Presentation of scmos in IsCMOS Sub-System. Jiarui GAO XIOPM, CAS
5 th HERD workshop CERN Presentation of scmos in IsCMOS Sub-System Jiarui GAO XIOPM, CAS 20171011 1 Outline Background scmos Design Next step 2 Background scmos is the readout module of IsCMOS. IsCMOS
More informationChapter 7. Widely Tunable Monolithic Laser Diodes
Chapter 7 Widely Tunable Monolithic Laser Diodes We have seen in Chapters 4 and 5 that the continuous tuning range λ is limited by λ/λ n/n g, where n is the index change and n g the group index of the
More informationGEM TPC Anode Pad Shape Studies
GEM TPC Anode Pad Shape Studies a,b, S. Kappler a,c, B. Ledermann a, Th. Müller a, M. Ronan d TPC-Application Workshop Berkeley, 04/08/2006 a b SLAC, Menlo Park, USA c RWTH, Aachen d LBNL, Berkeley, USA
More information6-1 LECTURE #6: OPTICAL PROPERTIES OF SOLIDS. Basic question: How do solids interact with light? The answers are linked to:
LECTURE #6: OPTICAL PROPERTIES OF SOLIDS Basic question: How do solids interact with light? The answers are linked to: Properties of light inside a solid Mechanisms behind light reflection, absorption
More informationTime-Resolved measurements by FEL spontaneous emission: A proposal for sub-picosecond pumps & probe structural and spectrometric investigations
Time-Resolved measurements by FEL spontaneous emission: A proposal for sub-picosecond pumps & probe structural and spectrometric investigations V. Rossi Albertini, B. Paci & P. Perfetti Istituto di Struttura
More informationResults of Radiation Test of the Cathode Front-end Board for CMS Endcap Muon Chambers
Results of Radiation Test of the Cathode Front-end Board for CMS Endcap Muon Chambers B. Bylsma 1, L.S. Durkin 1, J. Gu 1, T.Y. Ling 1, M. Tripathi 2 1 Department of Physics, Ohio State University, Columbus,
More informationISOTOPE IDENTIFICATION AND SOURCE DIRECTIONAL DETERMINATION USING GAMMA RADIATION PROFILING
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Theses, Dissertations, and Student Research from Electrical & Computer Engineering Electrical & Computer Engineering, Department
More informationDark Photon Search in e+e- Annihilation. MMAPS = Missing Mass A-Prime Search
Dark Photon Search in e+e- Annihilation MMAPS = Missing Mass A-Prime Search Cornell University J. Alexander, D. Cassel, M. Perelstein, D. Rubin, P. Wittich University of Minnesota Y. Kubota, B. Wojtsekhowski
More informationLASCAD Tutorial No. 2: Modeling a laser cavity with side pumped rod
LASCAD Tutorial No. 2: Modeling a laser cavity with side pumped rod Revised January 19, 2009 Copyright 2006-2009 LAS-CAD GmbH Table of Contents 1 Table of Contents 1 Starting LASCAD and Defining a Simple
More informationLECTURE 15. Dr. Teresa D. Golden University of North Texas Department of Chemistry
LECTURE 15 Dr. Teresa D. Golden University of North Texas Department of Chemistry Typical steps for acquisition, treatment, and storage of diffraction data includes: 1. Sample preparation (covered earlier)
More informationMonte Carlo Simulations for the Purpose of Efficiency Curve Calibration for the Fastscan Whole Body Counter
Monte Carlo Simulations for the Purpose of Efficiency Curve Calibration for the Fastscan Whole Body Counter by Hannah Robyn Graham A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE
More informationImplementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system
Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system 3 rd October 2008 11 th Topical Seminar on Innovative Particle and Radiation
More informationAccurate LED Source Modeling using TracePro
Accurate LED Source Modeling using TracePro Presented by : Lambda Research Corporation 25 Porter Rd. Littleton, MA 01460 Moderator: Mike Gauvin Vice President of Sales and Marketing Lambda Research Corporation
More informationLASERS FOR ANALYTICAL INSTRUMENTATION
CW Lasers Combiners Q-switch Lasers >20 s MM/SM/PM fiber Single-frequency options 405 nm to 660 nm 4 wavelengths Open beam or Fiber 1029 nm / 514.5 nm High pulse energy Single Longitudinal Mode LASERS
More informationFST s status on EUV Pellicle & Inspection System Development
FST s status on EUV Pellicle & Inspection System Development OCT.04, 2015 EUV Pellicle TWG @ Imec, nl. Donwon Park FST (Korea) http://www.fstc.co.kr FST Business Segments Division Pellicle TCU (Temperature
More informationSimulation of Internal Backscatter Effects on MTF and SNR of Pixelated Photon-counting Detectors
Simulation of Internal Backscatter Effects on MTF and SNR of Pixelated Photon-counting Detectors Alexander Korn, Juergen Giersch a and Martin Hoheisel b a Physikalisches Institut Universitaet Erlangen-Nuernberg,
More informationFluorescence. Requirements. Introduction. Models: FluorescenceExampleBegin.oml. Properties: FluorescenceExampleProperties.txt
Fluorescence Requirements Models: FluorescenceExampleBegin.oml Properties: FluorescenceExampleProperties.txt Editions: TracePro Expert Introduction TracePro Expert is capable of modeling fluorescent material.
More informationGEANT4 is used for simulating: RICH testbeam data, HCAL testbeam data. GAUSS Project: LHCb Simulation using GEANT4 with GAUDI.
Status of GEANT4 in LHCb S. Easo, RAL, 30-9-2002 The LHCbexperiment. GEANT4 is used for simulating: RICH testbeam data, HCAL testbeam data. GAUSS Project: LHCb Simulation using GEANT4 with GAUDI. Summary.
More informationSpherical Crystal X-ray Imaging for MTW, OMEGA, and OMEGA EP
Spherical Crystal X-ray Imaging for MTW, OMEGA, and OMEGA EP C.STOECKL, G. FISKEL, R. K. JUNGQUIST, P. M. NILSON, AND W. THEOBALD University of Rochester, Laboratory for Laser Energetics Spherical Crystal
More informationIDM-200 -V. Interchangeable HPGe Detector Module (IDM) for Systems Integrators
IDM-200 -V Interchangeable HPGe Detector Module (IDM) for Systems Integrators Free from liquid nitrogen, free from maintenance, free from integration complexities. Convenient-to-mount, all-in-one integrated
More informationDr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD (301) (301) fax
Dr. Larry J. Paxton Johns Hopkins University Applied Physics Laboratory Laurel, MD 20723 (301) 953-6871 (301) 953-6670 fax Understand the instrument. Be able to convert measured counts/pixel on-orbit into
More informationFT Cal and FT Hodo DAQ and Trigger
FT Cal and FT Hodo DAQ and Trigger Outline FT-Cal and FT-Hodo read-out electronics FT-Cal and FT-Hodo DAQ and trigger FADC250 firmware CTP firmware for FT-Cal and FT-Hodo FT-Cal and FT-Hodo crates and
More informationTPC digitization and track reconstruction: efficiency dependence on noise
TPC digitization and track reconstruction: efficiency dependence on noise Daniel Peterson, Cornell University, DESY, May-2007 A study of track reconstruction efficiency in a TPC using simulation of the
More informationDevelopment of a high resolution animal PET with continuous crystals and SiPMs
Development of a high resolution animal PET with continuous crystals and SiPMs 1, John Barrio1, Jorge Cabello1,2, Ane Etxebeste1, Carlos Lacasta1, Josep F. Oliver1, Magdalena Rafecas1, Carles Solaz1, Vera
More informationComparison of internal and external dose conversion factors using ICRP adult male and MEET Man voxel model phantoms.
Comparison of internal and external dose conversion factors using ICRP adult male and MEET Man voxel model phantoms. D.Leone, A.Häußler Intitute for Nuclear Waste Disposal, Karlsruhe Institute for Technology,
More informationGamma spectroscopic measurements using the PID350 pixelated CdTe radiation detector
Gamma spectroscopic measurements using the PID350 pixelated CdTe radiation detector K. Karafasoulis, K. Zachariadou, S. Seferlis, I. Papadakis, D. Loukas, C. Lambropoulos, C. Potiriadis Abstract Spectroscopic
More informationA full digital approach in Physics Applications
A full digital approach in Physics Applications March 2015 Carlo Tintori ISO 9001:2008 CERT. N. 9105.CAEN CAEN Digitizers Highlights VME, NIM, Desktop form factors Up to 64 channels in a single board 8,
More informationWAVELENGTH MANAGEMENT
BEAM DIAGNOS TICS SPECIAL PRODUCTS OEM DETECTORS THZ DETECTORS PHOTO DETECTORS HIGH POWER SOLUTIONS POWER DETECTORS ENERGY DETECTORS MONITORS Camera Accessories WAVELENGTH MANAGEMENT UV CONVERTERS UV Converters
More informationText for the class, Pump and probe technique for picosecond time-resolved x-ray diffraction at the Cheiron School
Yoshihito Tanaka, Kiminori Ito Oct. 3-4, 2011 Text for the class, Pump and probe technique for picosecond time-resolved x-ray diffraction at the Cheiron School 1. Introduction 1-1. Purpose The pulsed nature
More information